Difference between revisions of "Symmetric channel"
Ulf Rehmann (talk | contribs) m (tex encoded by computer) |
(details) |
||
(2 intermediate revisions by one other user not shown) | |||
Line 19: | Line 19: | ||
q ( y, \widetilde{y} ) = \ | q ( y, \widetilde{y} ) = \ | ||
\left \{ | \left \{ | ||
+ | |||
+ | \begin{array}{ll} | ||
+ | q & \textrm{ when } y = \widetilde{y} , \\ | ||
+ | |||
+ | \frac{1 - q }{n - 1 } | ||
+ | & \textrm{ when } y \neq \widetilde{y} , \\ | ||
+ | \end{array} | ||
+ | |||
+ | \right .$$ | ||
where $ n $ | where $ n $ | ||
Line 26: | Line 35: | ||
$$ | $$ | ||
− | \left \| | + | \left \| |
+ | \begin{array}{cc} | ||
+ | q &1 - q \\ | ||
+ | 1 - q & q \\ | ||
+ | \end{array} | ||
+ | \ | ||
+ | \right \| . | ||
+ | $$ | ||
For symmetric channels, many important information-theoretic characteristics can either be calculated explicitly or their calculation can be substantially simplified in comparison with non-symmetric channels. For example, for a memoryless symmetric channel with matrix $ \{ q ( y, \widetilde{y} ) : y, \widetilde{y} \in Y \} $ | For symmetric channels, many important information-theoretic characteristics can either be calculated explicitly or their calculation can be substantially simplified in comparison with non-symmetric channels. For example, for a memoryless symmetric channel with matrix $ \{ q ( y, \widetilde{y} ) : y, \widetilde{y} \in Y \} $ | ||
Line 40: | Line 56: | ||
For references see , | For references see , | ||
− | cited under [[ | + | cited under [[Communication channel]]. |
− | |||
− | |||
====References==== | ====References==== | ||
− | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> R.C. Gallager, "Information theory and reliable communication" , Wiley (1968)</TD></TR></table> | + | <table> |
+ | <TR><TD valign="top">[a1]</TD> <TD valign="top"> R.C. Gallager, "Information theory and reliable communication" , Wiley (1968)</TD></TR> | ||
+ | </table> |
Latest revision as of 08:59, 10 April 2023
A communication channel whose transition function possesses some kind of symmetry. A homogeneous discrete time memoryless channel with finite alphabets $ Y $
and $ \widetilde{Y} = Y $
of input and output letters, respectively, and defined by a matrix of transition probabilities $ \{ q ( y, \widetilde{y} ) : y, \widetilde{y} \in Y \} $
is called a symmetric channel if:
$$ \tag{* } q ( y, \widetilde{y} ) = \ \left \{ \begin{array}{ll} q & \textrm{ when } y = \widetilde{y} , \\ \frac{1 - q }{n - 1 } & \textrm{ when } y \neq \widetilde{y} , \\ \end{array} \right .$$
where $ n $ is the number of elements of $ Y $, $ 0 \leq q \leq 1 $. The most studied example of a memoryless symmetric channel is the binary symmetric channel with matrix of transition probabilities
$$ \left \| \begin{array}{cc} q &1 - q \\ 1 - q & q \\ \end{array} \ \right \| . $$
For symmetric channels, many important information-theoretic characteristics can either be calculated explicitly or their calculation can be substantially simplified in comparison with non-symmetric channels. For example, for a memoryless symmetric channel with matrix $ \{ q ( y, \widetilde{y} ) : y, \widetilde{y} \in Y \} $ of the form (*) the capacity $ C $( cf. Transmission rate of a channel) is given by the equation
$$ C = \mathop{\rm log} n + q \mathop{\rm log} q + ( 1 - q) \mathop{\rm log} \frac{1 - q }{n - 1 } . $$
For references see ,
cited under Communication channel.
References
[a1] | R.C. Gallager, "Information theory and reliable communication" , Wiley (1968) |
Symmetric channel. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Symmetric_channel&oldid=48921